U.S. patent number 8,218,929 [Application Number 12/691,174] was granted by the patent office on 2012-07-10 for large effective area low attenuation optical fiber.
This patent grant is currently assigned to Corning Incorporated. Invention is credited to Scott Robertson Bickham, Ming-Jun Li.
United States Patent |
8,218,929 |
Bickham , et al. |
July 10, 2012 |
Large effective area low attenuation optical fiber
Abstract
Optical waveguide fiber that has large effective area and low
loss characteristics, such as low attenuation and low bend loss.
The optical waveguide fiber includes a dual trench design wherein
an annular region closer to the core is preferably doped with at
least one downdopant such as fluorine, which annular region is
surrounded by another annular region that preferably includes
closed, randomly dispersed voids.
Inventors: |
Bickham; Scott Robertson
(Corning, NY), Li; Ming-Jun (Horseheads, NY) |
Assignee: |
Corning Incorporated (Corning,
NY)
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Family
ID: |
42167518 |
Appl.
No.: |
12/691,174 |
Filed: |
January 21, 2010 |
Prior Publication Data
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Document
Identifier |
Publication Date |
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US 20100215329 A1 |
Aug 26, 2010 |
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Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
Issue Date |
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61155741 |
Feb 26, 2009 |
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Current U.S.
Class: |
385/127;
385/123 |
Current CPC
Class: |
G02B
6/02357 (20130101); G02B 6/02019 (20130101); G02B
6/02366 (20130101); G02B 6/03661 (20130101); G02B
6/0365 (20130101); G02B 6/02266 (20130101) |
Current International
Class: |
G02B
6/02 (20060101) |
Field of
Search: |
;385/123,126,127 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
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0260795 |
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Jul 1987 |
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EP |
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1 978 383 |
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Oct 2008 |
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EP |
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2008/106033 |
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Sep 2008 |
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WO |
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Other References
"Optical transmission fiber design evolution"; Li, et al; Journal
of Lightwave Technology; vol. 26; No. 9, May 1, 2008; p. 1079-1092.
cited by other .
"Ultra-low bending loss single-mode fiber for FTTH"; Li et al;
Journal of Lightwave Technology; vol. 27, No. 3, Feb. 1, 2009; p.
376-382. cited by other.
|
Primary Examiner: Hahm; Sarah
Attorney, Agent or Firm: Mason; Matthew J.
Parent Case Text
CROSS-REFERENCE TO RELATED APPLICATIONS
This application claims the benefit of, and priority to U.S.
Provisional Patent Application No. 61/155,741 filed on Feb. 26,
2009 entitled, "Large Effective Area Low Attenuation Optical
Fiber", the content of which is relied upon and incorporated herein
by reference in its entirety.
Claims
What is claimed is:
1. An optical fiber comprising: a glass core extending from a
centerline to a radius R.sub.1, wherein R.sub.1 is greater than
about 5 .mu.m; a glass cladding surrounding and in contact with the
core; wherein the cladding comprises: a first annular region
extending from the radius R.sub.1 to a radius R.sub.2, the first
annular region comprising a radial width W.sub.1=R.sub.2-R.sub.1; a
second annular region extending from the radius R.sub.2 to a radius
R.sub.3, the second annular region comprising a radial width
W.sub.2=R.sub.3-R.sub.2; a third annular region extending from the
radius R.sub.3 to a radius R.sub.4, the third annular region
comprising a radial width W.sub.3=R.sub.4-R.sub.3; and a fourth
annular region extending from the radius R.sub.4 to an outermost
glass radius R.sub.5; wherein the core comprises a maximum relative
refractive index, .DELTA..sub.0MAX, the second annular region
comprises a minimum relative refractive index, .DELTA..sub.2MIN,
and the third annular region comprises a minimum relative
refractive index, .DELTA..sub.3MIN, wherein
.DELTA..sub.0MAX>0>.DELTA..sub.2MIN>.DELTA..sub.3MIN; and
wherein the core and the cladding provide a fiber with cable cutoff
less than 1500 nm and an effective area at 1550 nm of greater than
130 .mu.m.sup.2.
2. The optical fiber of claim 1, wherein
0.3%>.DELTA..sub.0MAX>0.1%,
-0.1%>.DELTA..sub.2MIN>-0.5%, and
.DELTA..sub.3MIN<-0.7%.
3. The optical fiber of claim 1, wherein 6 .mu.m<R.sub.1<9
.mu.m, 10 .mu.m<R.sub.2<15 .mu.m, 16 .mu.m<R.sub.3<24
.mu.m, and 20 .mu.m<R.sub.4<30 .mu.m.
4. The optical fiber of claim 1, wherein 2 .mu.m<W.sub.1<10
.mu.m, 3 .mu.m<W.sub.2<15 .mu.m, and 1.5
.mu.m<W.sub.3<4.5 .mu.m.
5. The optical fiber of claim 1, wherein the second annular region
comprises fluorine and is void-free.
6. The optical fiber of claim 1, wherein the third annular region
comprises silica based glass with at least 50 closed randomly
dispersed voids situated therein, and (i) the mean distance between
the voids is less than 5000 nm, and (ii) at least 80% of the voids
have a maximum cross-sectional dimension Di of less than 1000
nm.
7. The optical fiber of claim 1, wherein the second annular region
comprises a profile volume V.sub.2, equal to:
.times..intg..times..DELTA..times..times..times..times.d
##EQU00003## wherein |V.sub.2| is at least 30%-.mu.m.sup.2.
8. The optical fiber of claim 1, wherein the core and the cladding
provide a fiber having an attenuation at 1550 nm of less than 0.19
dB/km.
9. The optical fiber of claim 1, wherein the core and the cladding
provide a fiber with an effective area at 1550 nm of greater than
150 .mu.m.sup.2.
10. The optical fiber of claim 1, wherein the core and the cladding
provide a fiber with a bend loss at 1550 nm of less than 1.0
dB/turn on a 20 mm diameter mandrel.
11. An optical fiber comprising: a glass core extending from a
centerline to a radius R.sub.1, wherein R.sub.1 is greater than
about 5 .mu.m; a glass cladding surrounding and in contact with the
core; wherein the cladding comprises: a first annular region
extending from the radius R.sub.1 to a radius R.sub.2, the first
annular region comprising a radial width W.sub.1=R.sub.2-R.sub.1; a
second annular region extending from the radius R.sub.2 to a radius
R.sub.3, the second annular region comprising a radial width
W.sub.2=R.sub.3-R.sub.2; a third annular region extending from the
radius R.sub.3 to an outermost glass radius R.sub.4; wherein the
core comprises a maximum relative refractive index,
.DELTA..sub.0MAX, the first annular region comprises a minimum
relative refractive index, .DELTA..sub.1MIN, and the second annular
region comprises a minimum relative refractive index,
.DELTA..sub.2MIN, wherein
.DELTA..sub.0MAX>0>.DELTA..sub.1MIN>.DELTA..sub.2MIN; and
wherein the core and the cladding provide a fiber with cable cutoff
less than 1500 nm, an attenuation at 1550 nm of less than 0.20
dB/km, and an effective area at 1550 nm of greater than 130
.mu.m.sup.2; and wherein the second annular region comprises silica
based glass with at least 50 closed randomly dispersed voids
situated therein, and (i) the mean distance between the voids is
less than 5000 nm, and (ii) at least 80% of the voids have a
maximum cross-sectional dimension Di of less than 1000 nm.
12. The optical fiber of claim 11, wherein
0.3%>.DELTA..sub.0MAX>0.1%,
-0.1%>.DELTA..sub.1MIN>-0.5%, and
.DELTA..sub.2MIN<-0.7%.
13. The optical fiber of claim 11, wherein 6 .mu.m<R.sub.1<9
.mu.m, 16 .mu.m<R.sub.2<24 .mu.m, and 20
.mu.m<R.sub.3<30 .mu.m.
14. The optical fiber of claim 11, wherein 3 .mu.m<W.sub.1<15
.mu.m and 1.5 .mu.m<W.sub.2<4.5 .mu.m.
15. The optical fiber of claim 11, wherein the first annular region
comprises fluorine and is void-free.
16. The optical fiber of claim 11, wherein the first annular region
comprises a profile volume V.sub.1, equal to:
.times..intg..times..DELTA..times..times..times..times.d
##EQU00004## wherein |V.sub.1| is at least 30%-.mu.m.sup.2.
17. The optical fiber of claim 11, wherein the core and the
cladding provide a fiber having an attenuation at 1550 nm of less
than 0.19 dB/km.
18. The optical fiber of claim 11, wherein the core and the
cladding provide a fiber with an effective area at 1550 nm of
greater than 150 .mu.m.sup.2.
19. The optical fiber of claim 11, wherein the core and the
cladding provide a fiber with a bend loss at 1550 nm of less than
1.0 dB/turn on a 20 mm diameter mandrel.
Description
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates generally to optical fiber, and
particularly to optical fibers that have large effective area and
low bend loss at 1550 nm.
2. Technical Background
Optical amplifier technology and wavelength division multiplexing
techniques are typically required in telecommunication systems that
provide high power transmissions for long distances. The definition
of high power and long distances is meaningful only in the context
of a particular telecommunication system wherein a bit rate, a bit
error rate, a multiplexing scheme, and perhaps optical amplifiers
are specified. There are additional factors, known to those skilled
in the art, which have impacted upon the definition of high power
and long distance. However, for most purposes, high power is an
optical power greater than about 10 mW. In some applications,
single power levels of 1 mW or less are still sensitive to
non-linear effects, so that the effective area is still an
important consideration in such lower power systems.
Generally, an optical waveguide fiber having a large effective area
(A.sub.eff) reduces non-linear optical effects, including
self-phase modulation, four-wave-mixing, cross-phase modulation,
and non-linear scattering processes, all of which can cause
degradation of signals in high powered systems.
On the other hand, an increase in effective area of an optical
waveguide fiber typically results in an increase in macrobending
induced losses which attenuate signal transmission through a fiber.
The macrobending losses become increasingly significant over long
(e.g., 100 km, or more) distances (or spacing between regenerators,
amplifiers, transmitters and/or receivers). Unfortunately, the
larger the effective area of a conventional optical fiber is, the
higher the macrobend induced losses because the core does not
provide sufficient confinement of the optical power.
SUMMARY OF THE INVENTION
One aspect of the invention is an optical fiber that includes a
glass core extending from a centerline to a radius R.sub.1, wherein
R.sub.1 is greater than about 5 .mu.m, and a glass cladding
surrounding and in contact with the core. The cladding includes a
first annular region extending from the radius R.sub.1 to a radius
R.sub.2, the first annular region having a radial width
W.sub.1=R.sub.2-R.sub.1. The cladding also includes a second
annular region extending from the radius R.sub.2 to a radius
R.sub.3, the second annular region having a radial width
W.sub.2=R.sub.3-R.sub.2. In addition, the cladding includes a third
annular region extending from the radius R.sub.3 to a radius
R.sub.4, the third annular region having a radial width
W.sub.3=R.sub.4-R.sub.3. The cladding further includes a fourth
annular region extending from the radius R.sub.4 to an outermost
glass radius R.sub.5. The core has a maximum relative refractive
index, .DELTA..sub.0MAX. The second annular region has a minimum
relative refractive index, .DELTA..sub.2MIN. The third annular
region has a minimum relative refractive index, .DELTA..sub.3MIN.
In addition,
.DELTA..sub.0MAX>0>.DELTA..sub.2MIN>.DELTA..sub.3MIN.
Moreover, the core and the cladding provide a fiber with cable
cutoff less than 1500 nm and an effective area at 1550 nm of
greater than 130 .mu.m.sup.2.
In another aspect, the present invention includes an optical fiber
that includes a glass core extending from a centerline to a radius
R.sub.1, wherein R.sub.1 is greater than about 5 .mu.m, and a glass
cladding surrounding and in contact with the core. The cladding
includes a first annular region extending from the radius R.sub.1
to a radius R.sub.2, the first annular region having a radial width
W.sub.1=R.sub.2-R.sub.1. The cladding also includes a second
annular region extending from the radius R.sub.2 to a radius
R.sub.3, the second annular region having a radial width
W.sub.2=R.sub.3-R.sub.2. In addition, the cladding includes a third
annular region extending from the radius R.sub.3 to an outermost
glass radius R.sub.4. The core has a maximum relative refractive
index, .DELTA..sub.0MAX. The first annular region has a minimum
relative refractive index, .DELTA..sub.1MIN. The second annular
region has a minimum relative refractive index, .DELTA..sub.2MIN.
In addition,
.DELTA..sub.0MAX>0>.DELTA..sub.1MIN>.DELTA..sub.2MIN.
Moreover, the core and the cladding provide a fiber with cable
cutoff less than 1500 nm, an attenuation at 1550 nm of less than
0.20 dB/km, and an effective area at 1550 nm of greater than 130
.mu.m.sup.2.
In yet another aspect, the present invention includes an optical
fiber that includes a glass core extending from a centerline to a
radius R.sub.1, wherein R.sub.1 is greater than about 5 .mu.m, and
a glass cladding surrounding and in contact with the core. The core
and the cladding provide a fiber with cable cutoff less than 1500
nm, an attenuation at 1550 nm of less than 0.20 dB/km, and an
effective area at 1550 nm of greater than 150 .mu.m.sup.2.
Additional features and advantages of the invention will be set
forth in the detailed description which follows, and in part will
be readily apparent to those skilled in the art from that
description or recognized by practicing the invention as described
herein, including the detailed description which follows, the
claims, as well as the appended drawings.
It is to be understood that both the foregoing general description
and the following detailed description present embodiments of the
invention, and are intended to provide an overview or framework for
understanding the nature and character of the invention as it is
claimed. The accompanying drawings are included to provide a
further understanding of the invention, and are incorporated into
and constitute a part of this specification. The drawings
illustrate various embodiments of the invention, and together with
the description serve to explain the principles and operations of
the invention.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a schematic cross-sectional view of an embodiment of an
optical waveguide fiber as disclosed herein;
FIG. 2 shows a relative refractive index profile of an embodiment
of an optical waveguide fiber as disclosed herein;
FIG. 3 is a schematic cross-sectional view of another embodiment of
an optical waveguide fiber as disclosed herein; and
FIG. 4 shows a relative refractive index profile of another
embodiment of an optical waveguide fiber as disclosed herein.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
Reference will now be made in detail to the present preferred
embodiments of the invention, examples of which are illustrated in
the accompanying drawings.
The "refractive index profile" is the relationship between
refractive index or relative refractive index and waveguide fiber
radius.
The "relative refractive index percent" is defined as
.DELTA.%=100.times.(n.sub.i.sup.2-n.sub.c.sup.2)/2n.sub.i.sup.2,
where n.sub.i is the maximum refractive index in region i, unless
otherwise specified, and n.sub.c is the average refractive index of
the outermost region of the cladding. As used herein, the relative
refractive index is represented by .DELTA. and its values are given
in units of "%", unless otherwise specified.
"Chromatic dispersion", herein referred to as "dispersion" unless
otherwise noted, of a waveguide fiber is the sum of the material
dispersion, the waveguide dispersion, and the inter-modal
dispersion. In the case of single mode waveguide fibers the
inter-modal dispersion is zero. Dispersion slope is the rate of
change of dispersion with respect to wavelength.
"Effective area" is defined as:
A.sub.eff=2.pi.(.intg.f.sup.2rdr).sup.2/(.intg.f.sup.4rdr), where
the integration limits are 0 to .infin., and f is the transverse
component of the electric field associated with light propagated in
the waveguide. As used herein, "effective area" or "A.sub.eff"
refers to optical effective area at a wavelength of 1550 nm unless
otherwise noted.
The term ".alpha.-profile" or "alpha profile" refers to a relative
refractive index profile, expressed in terms of .DELTA.(r) which is
in units of "%", where r is radius, which follows the equation,
.DELTA.(r)=.DELTA.(r.sub.o)(1-[|r-r.sub.o|/(r.sub.1-r.sub.o)].sup..alpha.-
), where r.sub.o is the point at which .DELTA.(r) is maximum,
r.sub.1 is the point at which .DELTA.(r) % is zero, and r is in the
range r.sub.i.ltoreq.r.ltoreq.r.sub.f, where .DELTA. is defined
above, r.sub.i is the initial point of the .alpha.-profile, r.sub.f
is the final point of the .alpha.-profile, and .alpha. is an
exponent which is a real number.
The mode field diameter (MFD) is measured using the Peterman II
method wherein, 2w=MFD, and w.sup.2=(2.intg.f.sup.2 r
dr/.intg.[df/dr].sup.2 r dr), the integral limits being 0 to
.infin..
The bend resistance of a waveguide fiber can be gauged by induced
attenuation under prescribed test conditions, for example by
deploying or wrapping the fiber around a mandrel of a prescribed
diameter.
The cabled cutoff wavelength, or "cabled cutoff" is approximated by
the test described in the EIA-445 Fiber Optic Test Procedures,
which are part of the EIA-TIA Fiber Optics Standards, that is, the
Electronics Industry Alliance-Telecommunications Industry
Association Fiber Optics Standards, more commonly known as FOTP's.
Cabled cutoff measurement is described in EIA-455-170 Cable Cutoff
Wavelength of Single-mode Fiber by Transmitted Power, or
"FOTP-170". By cable cutoff as used herein, we mean the value
obtained using the approximated test.
"Kappa" or .kappa. is total dispersion divided by total dispersion
slope, both at 1550 nm.
Unless otherwise noted herein, optical properties (such as
dispersion, dispersion slope, etc.) are reported for the LP01 mode.
Unless otherwise noted herein, a wavelength of 1550 nm is the
reference wavelength.
Referring to FIGS. 1-2, in a set of preferred embodiments, optical
fiber 10 disclosed herein comprises a core 20 and a cladding layer
(or cladding) 200 surrounding and directly adjacent to the core.
The core 20 has a refractive index profile .DELTA..sub.CORE(r). The
cladding 200 has a refractive index profile
.DELTA..sub.CLAD(r).
In some embodiments, the core comprises silica doped with
germanium, i.e., germania doped silica. Dopants other than
germanium, singly or in combination, may be employed within the
core, and particularly at or near the centerline of the optical
fiber disclosed herein to obtain the desired refractive index and
density. In some embodiments, the optical fiber 10 contains no
index-decreasing dopants in the core 20.
Referring to FIGS. 1-2, optical waveguide fibers are disclosed
herein that include a core 20 extending radially outwardly from the
centerline to a radius R.sub.1 and having a relative refractive
index profile .DELTA..sub.0(r) in %, with a maximum relative
refractive index percent, .DELTA..sub.0MAX, and a cladding 200
surrounding and directly adjacent, i.e., in direct contact with,
the core 20. Cladding 200 includes a first annular region 30
extending from the radius R.sub.1 to a radius R.sub.2, the first
annular region having a radial width W.sub.1=R.sub.2-R.sub.1, a
midpoint R.sub.2MID=(R.sub.2+R.sub.1)/2, and a relative refractive
index profile .DELTA..sub.1(r) in %, with a midpoint relative
refractive index percent, .DELTA..sub.1MID, at R.sub.2MID, maximum
relative refractive index percent, .DELTA..sub.1MAX, and a minimum
relative refractive index percent .DELTA..sub.1MIN. Cladding 200
also includes a second annular region 40 extending from the radius
R.sub.2 to a radius R.sub.3, the second annular region having a
radial width W.sub.2=R.sub.3-R.sub.2 and a relative refractive
index profile .DELTA..sub.2(r) in %, with a minimum relative
refractive index percent .DELTA..sub.2MIN. Cladding 200
additionally includes a third annular region 50 extending from the
radius R.sub.3 to a radius R.sub.4, the third annular region having
a radial width W.sub.3=R.sub.4-R.sub.3, and a relative refractive
index profile .DELTA..sub.3(r) in %, with a minimum relative
refractive index percent .DELTA..sub.3MIN. Cladding 200 further
includes a fourth annular region 60 extending from the radius
R.sub.4 to the outermost glass radius R.sub.5, having a relative
refractive index profile .DELTA..sub.4(r) in %. Fourth annular
region 60 can be optionally surrounded by one or more polymer
coatings 65. R.sub.1 is defined to occur at the radius where
.DELTA..sub.0(r) first reaches 0.03% going radially outward from
the centerline. That is, core 20 ends and the first annular region
30 begins where the relative refractive index first reaches 0.03%
(going radially outward) at a radius R.sub.1. R.sub.2 is defined to
occur at the radius where .DELTA..sub.1(r) first reaches -0.05%
going radially outward from R.sub.1. That is, first annular region
30 ends and second annular region 40 begins where the relative
refractive index first reaches -0.05% (going radially outward) at a
radius R.sub.2. R.sub.3 is defined to occur at the radius where
.DELTA..sub.2(r) first reaches -0.5% going radially outward from
R.sub.2. That is, second annular region 40 ends and third annular
region 50 begins where the relative refractive index first reaches
-0.5% (going radially outward) at a radius R.sub.3. R.sub.4 is
defined to occur at the radius where .DELTA..sub.4(r) first reaches
-0.05% going radially inward from R.sub.5. That is, fourth annular
region 60 ends and third annular region 50 begins where the
relative refractive index first reaches -0.05% (going radially
inward) at a radius R.sub.4. R.sub.1 is greater than about 5 .mu.m.
Also,
.DELTA..sub.0MAX>0>.DELTA..sub.2MIN>.DELTA..sub.3MIN. In
addition,
.DELTA..sub.0MAX>.DELTA..sub.1MAX>.DELTA..sub.1MID>.DE-
LTA..sub.1MIN>.DELTA..sub.2MIN>.DELTA..sub.3MIN.
The second annular region 40 has a profile volume, V.sub.2, defined
herein as:
.times..intg..times..DELTA..times..times..function..times..times.d
##EQU00001##
In preferred embodiments, .DELTA..sub.0MAX<0.3%, such as
0.3%>.DELTA..sub.0MAX>0.1% and
0.25%>.DELTA..sub.0MAX>0.1%, .DELTA..sub.2MIN<-0.1%, such
as -0.1%>.DELTA..sub.2MIN>-0.5%, and
.DELTA..sub.3MIN<-0.5%, such as -0.7%>.DELTA..sub.3MIN>-3%
and -0.7%>.DELTA..sub.3MIN>-2%. Preferably, .DELTA..sub.1MAX
is not greater than 0.03%, .DELTA..sub.1MIN is not less than
-0.03%, and 0.025%>.DELTA..sub.1MID>-0.025%. Preferably,
R.sub.1>6 .mu.m, such as 6 .mu.m<R.sub.1<9 .mu.m,
R.sub.2>10 .mu.m, such as 10 .mu.m<R.sub.2<15 .mu.m,
R.sub.3>16 .mu.m, such as 16 .mu.m<R.sub.3<24 .mu.m, and
R.sub.4>20 .mu.m, such as 20 .mu.m<R.sub.4<30 .mu.m.
Preferably, W.sub.1>2 .mu.m, such as 2 .mu.m<W.sub.1<10
.mu.m, W.sub.2>3 .mu.m, such as 3 .mu.m<W.sub.2<15 .mu.m,
and W.sub.3>1.5 .mu.m, such as 1.5 .mu.m<W.sub.3<4.5
.mu.m. Preferably, |V.sub.2| is at least 30%-.mu.m.sup.2, such as
30%-.mu.m.sup.2<|V.sub.2|<90%-.mu.m.sup.2 and further such as
40%-.mu.m.sup.2<|V.sub.2|<80%-.mu.m.sup.2.
In preferred embodiments, .DELTA..sub.2MIN<-0.25%, such as
-0.3%>.DELTA..sub.2MIN>-0.5%, and W.sub.1>5 .mu.m, such as
6 .mu.m<W.sub.1<10 .mu.m. Preferably,
.DELTA..sub.0MAX<0.3%, such as 0.3%>.DELTA..sub.0MAX>0.1%,
and .DELTA..sub.3MIN<-0.7%, such as
-0.7%>.DELTA..sub.3MIN>-3% and
-0.7%>.DELTA..sub.3MIN>-2%. Preferably, .DELTA..sub.1MAX is
not greater than 0.05%, .DELTA..sub.1MIN is not less than -0.05%,
and 0.025%>.DELTA..sub.1MID>-0.025%. Preferably, R.sub.1>6
.mu.m, such as 6 .mu.m<R.sub.1<9 .mu.m, R.sub.2>12 .mu.m,
such as 12 .mu.m<R.sub.2<15 .mu.m, R.sub.3>16 .mu.m, such
as 16 .mu.m<R.sub.3<24 .mu.m, and R.sub.4>20 .mu.m, such
as 20 .mu.m<R.sub.4<30 .mu.m. Preferably, W.sub.2>3 .mu.m,
such as 3 .mu.m<W.sub.2<9 .mu.m, and W.sub.3>1.5 .mu.m,
such as 1.5 .mu.m<W.sub.3<4.5 .mu.m. Preferably, |V.sub.2| is
at least 30%-.mu.m.sup.2, such as
30%-.mu.m.sup.2<|V.sub.2|<90%-.mu.m.sup.2 and further such as
40%-.mu.m.sup.2<|V.sub.2|<80%-.mu.m.sup.2.
In preferred embodiments, .DELTA..sub.2MIN>-0.25%, such as
-0.1%>.DELTA..sub.2MIN>-0.25%, W.sub.1<5 .mu.m, such as 2
.mu.m<W.sub.1<4 .mu.m, and W.sub.2>5 .mu.m, such as 6
.mu.m<W.sub.2<15 .mu.m. Preferably, .DELTA..sub.0MAX<0.3%,
such as 0.3%>.DELTA..sub.0MAX>0.1%, and
.DELTA..sub.3MIN<-0.7%, such as
-0.7%>.DELTA..sub.3MIN>-3%. Preferably, .DELTA..sub.1MAX is
not greater than 0.03%, .DELTA..sub.1MIN is not less than -0.03%,
and 0.025%>.DELTA..sub.1MID>-0.025%. Preferably, R.sub.1>6
.mu.m, such as 6 .mu.m<R.sub.1<9 .mu.m, R.sub.2>10 .mu.m,
such as 10 .mu.m<R.sub.2<13 .mu.m, R.sub.3>16 .mu.m, such
as 16 .mu.m<R.sub.3<24 .mu.m, and R.sub.4>20 .mu.m, such
as 20 .mu.m<R.sub.4<30 .mu.m. Preferably, W.sub.3>1.5
.mu.m, such as 1.5 .mu.m<W.sub.3<4.5 .mu.m. Preferably,
|V.sub.2| is at least 30%-.mu.m.sup.2, such as
30%-.mu.m.sup.2<|V.sub.2|90%-.mu.m.sup.2 and further such as
40%.mu.m.sup.2<|V.sub.2|<80%-.mu.m.sup.2.
In preferred embodiments, second annular region 40 comprises silica
glass having at least one dopant selected from the group consisting
of germanium, aluminum, phosphorous, titanium, boron, and fluorine.
In more preferred embodiments, second annular region 40 consists
essentially of silica glass having at least one dopant selected
from the group consisting of boron and fluorine. In even more
preferred embodiments, second annular region 40 consists
essentially of silica glass doped with fluorine. Preferably, second
annular region 40 contains no voids (i.e., is void-free).
Referring specifically to FIG. 1, the third annular region 50
preferably comprises silica based glass (either pure, undoped
silica or silica doped with for example, at least one of germanium,
aluminum, phosphorous, titanium, boron, and fluorine) containing a
plurality of closed randomly dispersed voids 16A, the voids 16A
being either empty (vacuum) or containing a gas (e.g., argon, air,
nitrogen, krypton, or SO.sub.2) filled. Such voids can provide an
effective refractive index which is low, e.g., compared to pure
silica. The relative percent index of refraction (.DELTA.n %) in
third annular region 50 fluctuates between -28% (index of void
filled gas relative to that of silica) and that of the glass
surrounding the voids (in this example it is silica, with the
relative % index of refraction .DELTA..sub.4(r) of about 0%). A
typical average relative refractive index percent .DELTA..sub.3avg
of the third annular region 50 will be between -1% and -3%,
relative to pure silica glass, depending on the dopants present in
the glass surrounding the voids. That is, the index of third
annular region 50 fluctuates, and in the example of FIG. 1 the
width of the gas filled voids, and/or the glass filled spacing
S.sub.v between the gas filled voids is randomly distributed and/or
are not equal to one another. That is, the voids are non-periodic.
It is preferable that the mean distance between the voids is less
than 5000 nm, more preferably less than 2000 nm, even more
preferably less than 1000 nm, for example less than 750 nm, 500 nm,
400 nm, 300 nm, 200 nm or 100 nm. Preferably, at least 80%, and
more preferably at least 90% of the voids have a maximum
cross-sectional dimension Di of less than 1000 nm, preferably less
than 500 nm. Even more preferably, the mean diameter of the voids
is less than 500 nm, more preferably less than 300 nm, and even
more preferably less than 200 nm. The voids 16A are closed
(surrounded by solid material) and are non-periodic. That is, the
voids 16A may have the same size, or may be of different sizes. The
distances between voids may be uniform (i.e., the same), or may be
different. Preferably the third annular region 50 when viewed in
cross section exhibits at least 50 voids, more preferably at least
100 voids, even more preferably at least 200 voids and most
preferably at least 250 voids.
In some embodiments, a central segment of the core 20 may comprise
a relative refractive index profile having a so-called centerline
dip which may occur as a result of one or more optical fiber
manufacturing techniques. For example, the central segment may have
a local minimum in the refractive index profile at radii less than
1 .mu.m, wherein higher values for the relative refractive index
(including the maximum relative refractive index for the core
segment) occur at radii greater than r=0 .mu.m.
Referring to FIGS. 3-4, optical waveguide fibers 110 are disclosed
herein that include a core 120 extending radially outwardly from
the centerline to a radius R.sub.1 and having a relative refractive
index profile .DELTA..sub.0(r) in %, with a maximum relative
refractive index percent, .DELTA..sub.0MAX, and a cladding 300
surrounding and directly adjacent, i.e., in direct contact with,
the core 120. Cladding 300 includes a first annular region 140
extending from the radius R.sub.1 to a radius R.sub.2, the first
annular region having a radial width W.sub.1=R.sub.2-R.sub.1 and a
relative refractive index profile .DELTA..sub.1(r) in %, with a
minimum relative refractive index percent .DELTA..sub.1MIN.
Cladding 300 also includes a second annular region 150 extending
from the radius R.sub.2 to a radius R.sub.3, the second annular
region having a radial width W.sub.2=R.sub.3-R.sub.2, and a
relative refractive index profile .DELTA..sub.2(r) in %, with a
minimum relative refractive index percent .DELTA..sub.2MIN.
Cladding 300 additionally includes a third annular region 160
extending from the radius R.sub.3 to the outermost glass radius
R.sub.4, having a relative refractive index profile
.DELTA..sub.3(r) in %. Third annular region 160 can be optionally
surrounded by one or more polymer coatings 165. R.sub.1 is defined
to occur at the radius where .DELTA..sub.0(r) first reaches 0%
going radially outward from the centerline. That is, core 120 ends
and the first annular region 140 begins where the relative
refractive index first reaches 0% (going radially outward) at a
radius R.sub.1. R.sub.2 is defined to occur at the radius where
.DELTA..sub.1(r) first reaches -0.5% going radially outward from
R.sub.1. That is, first annular region 140 ends and second annular
region 150 begins where the relative refractive index first reaches
-0.5% (going radially outward) at a radius R.sub.2. R.sub.3 is
defined to occur at the radius where .DELTA..sub.3(r) first reaches
-0.05% going radially inward from R.sub.4. That is, third annular
region 160 ends and second annular region 150 begins where the
relative refractive index first reaches -0.05% (going radially
inward) at a radius R.sub.3. R.sub.1 is greater than about 5 .mu.m.
Also,
.DELTA..sub.0MAX>0>.DELTA..sub.1MIN>.DELTA..sub.2MIN.
The first annular region 140 has a profile volume, V.sub.1, defined
herein as:
.times..intg..times..DELTA..times..times..times..times.d
##EQU00002##
In preferred embodiments, .DELTA..sub.0MAX<0.3%, such as
0.3%>.DELTA..sub.0MAX>0.1% and
0.25%>.DELTA..sub.0MAX>0.1%, .DELTA..sub.1MIN<-0.1%, such
as -0.1%>.DELTA..sub.1MIN>-0.5%, and
.DELTA..sub.2MIN<-0.7%, such as -0.7%>.DELTA..sub.2MIN>-3%
and 0.7%>.DELTA..sub.2MIN>-2%. Preferably, R.sub.1>6
.mu.m, such as 6 .mu.m<R.sub.1<9 .mu.m, R.sub.2>16 .mu.m,
such as 16 .mu.m<R.sub.2<24 .mu.m, and R.sub.3>20 .mu.m,
such as 20 .mu.m<R.sub.3<30 .mu.m. Preferably, W.sub.1>3
.mu.m, such as 3 .mu.m<W.sub.1<15 .mu.m, and W.sub.2>1.5
.mu.m, such as 1.5 .mu.m<W.sub.2<4.5 .mu.m. Preferably,
|V.sub.1| is at least 30%-.mu.m.sup.2, such as
30%-.mu.m.sup.2<|V.sub.1|<90%-.mu.m.sup.2 and further such as
40%-.mu.m.sup.2<|V.sub.1|<80%-.mu.m.sup.2.
In preferred embodiments, first annular region 140 comprises silica
glass having at least one dopant selected from the group consisting
of germanium, aluminum, phosphorous, titanium, boron, and fluorine.
In more preferred embodiments, first annular region 140 consists
essentially of silica glass having at least one dopant selected
from the group consisting of boron and fluorine. In even more
preferred embodiments, first annular region 140 consists
essentially of silica glass doped with fluorine. Preferably, first
annular region 140 contains no voids (i.e., is void-free).
Referring specifically to FIG. 3, the second annular region 150
preferably comprises silica based glass (either pure, undoped
silica or silica doped with for example, at least one of germanium,
aluminum, phosphorous, titanium, boron, and fluorine) containing a
plurality of closed randomly dispersed voids 116A, the voids 116A
being either empty (vacuum) or containing a gas (e.g., argon, air,
nitrogen, krypton, or SO.sub.2) filled. Such voids can provide an
effective refractive index which is low, e.g., compared to pure
silica. The relative percent index of refraction (.DELTA.n %) in
second annular region 150 fluctuates between -28% (index of void
filled gas relative to that of silica) and that of the glass
surrounding the voids (in this example it is silica, with the
relative % index of refraction .DELTA..sub.4(r) of about 0%). A
typical average relative refractive index percent .DELTA..sub.3avg
of the second annular region 150 will be between -1% and -3%,
relative to pure silica glass, depending on the dopants present in
the glass surrounding the voids. That is, the index second annular
region 150 fluctuates, and in the example of FIG. 3 the width of
the gas filled voids, and/or the glass filled spacing S.sub.v
between the gas filled voids is randomly distributed and/or are not
equal to one another. That is, the voids are non-periodic. It is
preferable that the mean distance between the voids is less than
5000 nm, more preferably less than 2000 nm, even more preferably
less than 1000 nm, for example less than 750 nm, 500 nm, 400 nm,
300 nm, 200 nm or 100 nm. Preferably, at least 80%, and more
preferably at least 90% of the voids have a maximum cross-sectional
dimension Di of less than 1000 nm, preferably less than 500 nm.
Even more preferably, the mean diameter of the voids is less than
500 nm, more preferably less than 300 nm, and even more preferably
less than 200 nm. The voids 116A are closed (surrounded by solid
material) and are non-periodic. That is, the voids 116A may have
the same size, or may be of different sizes. The distances between
voids may be uniform (i.e., the same), or may be different.
Preferably the second annular region 150 when viewed in cross
section exhibits at least 50 voids, more preferably at least 100
voids, even more preferably at least 200 voids and most preferably
at least 250 voids.
In some embodiments, a central segment of the core 120 may comprise
a relative refractive index profile having a so-called centerline
dip which may occur as a result of one or more optical fiber
manufacturing techniques. For example, the central segment may have
a local minimum in the refractive index profile at radii less than
1 .mu.m, wherein higher values for the relative refractive index
(including the maximum relative refractive index for the core
segment) occur at radii greater than r=0 .mu.m.
The embodiments disclosed herein provide a dual trench design,
wherein an annular region closer to the core is preferably doped
with at least one downdopant such as fluorine, which annular region
is surrounded by another annular region that preferably includes
closed, randomly dispersed voids. This dual trench design has been
found to provide for an optical fiber having a combination of large
effective area and low loss characteristics. In particular, this
dual trench design has been found to provide an optical fiber with
a cable cutoff of less than 1500 nm and an effective area at 1550
nm of greater than 130 .mu.m.sup.2, such as an effective area of
130 .mu.m.sup.2 to 200 .mu.m.sup.2, wherein the fiber also has low
attenuation and low microbend loss.
Preferably, optical fiber disclosed herein provide a cable cutoff
of less than 1450 nm, including a cable cutoff of less than 1400
nm. Preferably, optical fiber disclosed herein provide an effective
area at 1550 nm of greater than 140 .mu.m.sup.2, such as an
effective area of 140 .mu.m.sup.2 to 190 .mu.m.sup.2. More
preferably, optical fiber disclosed herein provide an effective
area at 1550 nm of greater than 150 .mu.m.sup.2, such as an
effective area of 150 .mu.m.sup.2 to 180 .mu.m.sup.2. Preferably,
optical fiber disclosed herein provide an attenuation at 1550 nm of
less than 0.21 dB/km, even more preferably less than 0.20 dB/km,
and yet even more preferably less than 0.19 dB/km. Preferably,
optical fiber disclosed herein provide a bend loss at 1550 nm of
less than 1.5 dB/turn around a 20 mm diameter mandrel, even more
preferably a bend loss at 1550 nm of less than 1.0 dB/turn around a
20 mm diameter mandrel, and yet even more preferably a bend loss at
1550 nm of less than 0.5 dB/turn around a 20 mm diameter
mandrel.
EXAMPLES
Examples 1-5 set forth refractive index profile parameters and
optical properties of modeled optical fibers in accordance with
embodiments disclosed herein and illustrated, for example, in FIGS.
1-2. Table 1 lists refractive index profile parameters of Examples
1-5 and Table 2 lists modeled optical properties of Examples
1-5.
TABLE-US-00001 TABLE 1 Refractive Index Profile Parameters Example
1 2 3 4 5 .DELTA..sub.0MAX (%) 0.2 0.198 0.198 0.196 0.16 R.sub.1
(.mu.m) 7.17 7.17 7.3 7.3 8.15 .DELTA..sub.1MID (%) 0 0 0 0 0
R.sub.2 (.mu.m) 14.5 12.4 11.45 11.1 12.1 W.sub.1 (.mu.m) 7.33 5.23
4.15 3.8 3.95 .DELTA..sub.2MIN (%) -0.4 -0.3 -0.25 -0.18 -0.18
R.sub.3 (.mu.m) 19.5 19.5 19.5 21 22 W.sub.2 (.mu.m) 5 7.1 8.05 9.9
9.9 .DELTA..sub.3MIN (%) -1 -1 -1 -1 -1.3 R.sub.4 (.mu.m) 22 22 22
23 24 W.sub.3 (.mu.m) 2.5 2.5 2.5 2 2 core alpha 8 8 8 8 8
|V.sub.2| (%-.mu.m.sup.2) 68 67.9 62.3 57.2 60.8
TABLE-US-00002 TABLE 2 Modeled Optical Properties Example 1 2 3 4 5
MFD at 1550 nm 13.94 13.74 13.67 13.72 15.11 (.mu.m) Aeff at 1550
nm 153.0 150.1 150.0 150.9 184.2 (.mu.m.sup.2) Dispersion at 1550
20.92 21.39 21.68 21.56 21.83 nm (ps/nm/km) Dispersion Slope 0.0643
0.0647 0.0647 0.0643 0.0646 at 1550 nm (ps/nm.sup.2/km) Kappa at
1550 nm 325.3 330.4 335.3 335.4 337.9 (nm) LP11 Cutoff (nm) 1423
1391 1398 1392 1393 Attenuation at 0.1846 0.1845 0.1845 0.1844
0.1831 1550 nm (dB/km)
Each of the modeled optical fibers of Examples 1-5 is expected to
exhibit a bend loss at 1550 nm of less than 1.0 dB/turn around a 20
mm diameter mandrel.
It will be apparent to those skilled in the art that various
modifications and variations can be made to the present invention
without departing from the spirit and scope of the invention. Thus
it is intended that the present invention cover the modifications
and variations of this invention provided they come within the
scope of the appended claims and their equivalents.
* * * * *